Jump to
S1C2
S1C3
Energy calculated at wB97X-D/cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.786483 |
| Energy at 298.15K | |
| HF Energy | -1592.786483 |
| Nuclear repulsion energy | 351.203947 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at wB97X-D/cc-pVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
544 |
520 |
0.00 |
41.60 |
0.05 |
0.09 |
| 2 |
A1 |
202 |
193 |
0.00 |
2.35 |
0.75 |
0.85 |
| 3 |
B1 |
490 |
469 |
0.00 |
17.73 |
0.75 |
0.86 |
| 4 |
B2 |
306 |
293 |
0.00 |
8.26 |
0.75 |
0.86 |
| 5 |
E |
465 |
445 |
0.00 |
4.44 |
0.75 |
0.86 |
| 5 |
E |
465 |
445 |
0.00 |
4.44 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1235.8 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 1181.5 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at wB97X-D/cc-pVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.429 |
0.309 |
| S2 |
0.000 |
-1.429 |
0.309 |
| S3 |
-1.429 |
0.000 |
-0.309 |
| S4 |
1.429 |
0.000 |
-0.309 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8580 | 2.1134 | 2.1134 |
S2 | 2.8580 | | 2.1134 | 2.1134 | S3 | 2.1134 | 2.1134 | | 2.8580 | S4 | 2.1134 | 2.1134 | 2.8580 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.456 |
|
S1 |
S3 |
S4 |
47.456 |
| S2 |
S1 |
S3 |
47.456 |
|
S2 |
S4 |
S3 |
47.456 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.000 |
|
|
|
| 2 |
S |
0.000 |
|
|
|
| 3 |
S |
0.000 |
|
|
|
| 4 |
S |
0.000 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.579 |
0.000 |
0.000 |
| y |
0.000 |
-48.579 |
0.000 |
| z |
0.000 |
0.000 |
-54.090 |
|
| Traceless |
| | x | y | z |
| x |
2.755 |
0.000 |
0.000 |
| y |
0.000 |
2.755 |
0.000 |
| z |
0.000 |
0.000 |
-5.511 |
|
| Polar |
| 3z2-r2 | -11.021 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
11.327 |
0.000 |
0.000 |
| y |
0.000 |
11.327 |
0.000 |
| z |
0.000 |
0.000 |
6.564 |
<r2> (average value of r
2) Å
2
| <r2> |
168.295 |
| (<r2>)1/2 |
12.973 |
Jump to
S1C1
S1C3
Energy calculated at wB97X-D/cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.797198 |
| Energy at 298.15K | |
| HF Energy | -1592.797198 |
| Nuclear repulsion energy | 334.424074 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at wB97X-D/cc-pVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
693 |
662 |
7.59 |
27.43 |
0.14 |
0.25 |
| 2 |
A1 |
444 |
424 |
5.70 |
54.56 |
0.20 |
0.33 |
| 3 |
A1 |
137 |
131 |
0.36 |
14.49 |
0.43 |
0.60 |
| 4 |
A2 |
220 |
210 |
0.00 |
0.19 |
0.75 |
0.86 |
| 5 |
B2 |
659 |
630 |
154.92 |
4.05 |
0.75 |
0.86 |
| 6 |
B2 |
348 |
333 |
0.52 |
11.62 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1250.2 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 1195.2 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at wB97X-D/cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.034 |
0.911 |
| S2 |
0.000 |
-1.034 |
0.911 |
| S3 |
0.000 |
1.600 |
-0.911 |
| S4 |
0.000 |
-1.600 |
-0.911 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0683 | 1.9078 | 3.2031 |
S2 | 2.0683 | | 3.2031 | 1.9078 | S3 | 1.9078 | 3.2031 | | 3.2009 | S4 | 3.2031 | 1.9078 | 3.2009 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
107.268 |
|
S1 |
S3 |
S4 |
72.732 |
| S2 |
S1 |
S3 |
107.268 |
|
S2 |
S4 |
S3 |
72.732 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.150 |
|
|
|
| 2 |
S |
0.150 |
|
|
|
| 3 |
S |
-0.150 |
|
|
|
| 4 |
S |
-0.150 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
1.661 |
1.661 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-50.949 |
0.000 |
0.000 |
| y |
0.000 |
-53.237 |
0.000 |
| z |
0.000 |
0.000 |
-48.369 |
|
| Traceless |
| | x | y | z |
| x |
-0.146 |
0.000 |
0.000 |
| y |
0.000 |
-3.578 |
0.000 |
| z |
0.000 |
0.000 |
3.724 |
|
| Polar |
| 3z2-r2 | 7.448 |
| x2-y2 | 2.288 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.765 |
0.000 |
0.000 |
| y |
0.000 |
18.896 |
0.000 |
| z |
0.000 |
0.000 |
11.763 |
<r2> (average value of r
2) Å
2
| <r2> |
201.053 |
| (<r2>)1/2 |
14.179 |
Jump to
S1C1
S1C2
Energy calculated at wB97X-D/cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.786476 |
| Energy at 298.15K | |
| HF Energy | -1592.786476 |
| Nuclear repulsion energy | 339.992104 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at wB97X-D/cc-pVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
763 |
729 |
0.00 |
35.23 |
0.21 |
0.34 |
| 2 |
Ag |
309 |
295 |
0.00 |
47.51 |
0.25 |
0.40 |
| 3 |
Au |
264 |
253 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
693 |
663 |
158.52 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
225i |
215i |
25.11 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
356 |
340 |
0.00 |
14.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1079.9 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 1032.4 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at wB97X-D/cc-pVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.942 |
1.241 |
| S2 |
0.000 |
0.942 |
-1.241 |
| S3 |
0.000 |
-0.942 |
1.241 |
| S4 |
0.000 |
-0.942 |
-1.241 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.4812 | 1.8838 | 3.1153 |
S2 | 2.4812 | | 3.1153 | 1.8838 | S3 | 1.8838 | 3.1153 | | 2.4812 | S4 | 3.1153 | 1.8838 | 2.4812 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
90.000 |
|
S1 |
S3 |
S4 |
90.000 |
| S2 |
S1 |
S3 |
90.000 |
|
S2 |
S4 |
S3 |
90.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.000 |
|
|
|
| 2 |
S |
0.000 |
|
|
|
| 3 |
S |
0.000 |
|
|
|
| 4 |
S |
0.000 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.269 |
0.000 |
0.000 |
| y |
0.000 |
-47.622 |
0.000 |
| z |
0.000 |
0.000 |
-52.627 |
|
| Traceless |
| | x | y | z |
| x |
-1.145 |
0.000 |
0.000 |
| y |
0.000 |
4.326 |
0.000 |
| z |
0.000 |
0.000 |
-3.181 |
|
| Polar |
| 3z2-r2 | -6.363 |
| x2-y2 | -3.647 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.729 |
0.000 |
0.000 |
| y |
0.000 |
12.305 |
0.000 |
| z |
0.000 |
0.000 |
17.500 |
<r2> (average value of r
2) Å
2
| <r2> |
186.828 |
| (<r2>)1/2 |
13.669 |